Search results for "HYPERFINE"

showing 10 items of 428 documents

Hyperfine structure andg-factor measurements in ion traps

1992

We report about measurements on ground-state hyperfine splitting constants of stable Eu+ isotopes in radio frequency ion traps and experiments on the electronicg-factor of Ba+ in a Penning trap. From the precision of both measurements, which ranges between 3·10−6 and 5·10−7, we conclude that precise determination of the differential Bohr-Weisskopf effect in chains of isotopes will be possible in the near future.

PhysicsNuclear and High Energy PhysicsIsotopePhysics::Atomic PhysicsRadio frequencyPhysical and Theoretical ChemistryAtomic physicsCondensed Matter PhysicsPenning trapHyperfine structureAtomic and Molecular Physics and OpticsIonHyperfine Interactions
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Nuclear moments and charge radii of107?111in determined by laser spectroscopy

1985

Collinear fast beam laser spectroscopy has been used to measure the hyperfine structure and isotope shift in the atomic 5s 2 5p 2 P 3/2-5s 2 6s 2 S 1/2 transition (λ=451 nm) of107–111In. Secondary beams of neutron deficient indium isotopes were prepared at the GSI on-line mass separator following fusion evaporation reactions. Magnetic dipole moments and electric quadrupole moments have been determined. The isotope shifts are discussed in terms of the change of the mean square nuclear charge radii and compared with the droplet model predictions and the deformation values calculated from the quadrupole moments.

PhysicsNuclear and High Energy PhysicsIsotopeQuadrupoleNuclear fusionNeutronPhysics::Atomic PhysicsAtomic physicsNuclear ExperimentSpectroscopyHyperfine structureMagnetic dipoleEffective nuclear chargeZeitschrift f�r Physik A Atoms and Nuclei
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Laser-spectroscopy measurements of 72–96Kr spins, moments and charge radii

1994

Abstract The spins, moments and radii of krypton isotopes have been investigated by collinear fast-beam laser spectroscopy in combination with ultra-sensitive collisional ionization detection. The sequence of isotopes under study ranges from the neutron-deficient N = Z = 36 isotope 72 Kr to the neutron-rich 96 Kr ( N = 60). The mean-square charge radii in the neighbourhood of the N = 50 neutron-shell closure exhibit a pronounced shell effect which has recently been explained in the framework of relativistic mean-field theory. The results for the neutron-deficient nuclei are related to the shape coexistence of strongly prolate and near-spherical states which is known from nuclear spectroscop…

PhysicsNuclear and High Energy PhysicsIsotopeSpinsStable isotope ratioNuclear TheoryKryptonchemistry.chemical_elementchemistryNeutron numberIonizationNuclear Physics - ExperimentPhysics::Atomic PhysicsAtomic physicsNuclear ExperimentSpectroscopyHyperfine structureNuclear Physics A
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Nuclear moments and charge radii of bismuth isotopes

2000

Isotope shifts and hyperfine structures have been measured on the 306.7 nm line in bismuth isotopes with A = 205-210, 210m, 212 and 213 by gas cell laser spectroscopy. More precise measurements were made for the A = 207-209 isotopes in atomic beam measurements. Nuclear magnetic and quadrupole moments were deduced. A detailed comparison of the nuclear charge radii systematics has been made in the region using a King plot technique.

PhysicsNuclear and High Energy PhysicsIsotopechemistry.chemical_elementEffective nuclear chargeBismuthchemistryQuadrupolePhysics::Atomic PhysicsAtomic physicsNuclear ExperimentAtomic vapor laser isotope separationSpectroscopyHyperfine structureLine (formation)Journal of Physics G: Nuclear and Particle Physics
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Atomic beam magnetic resonance apparatus for systematic measurement of hyperfine structure anomalies (Bohr-Weisskopf effect)

1993

Abstract An atomic beam magnetic resonance (ABMR) apparatus has been constructed at Orsay, and has been installed at the CERN PS Booster ISOLDE mass separator facility for “on-line” work with radioactive isotopes in a program to measure hyperfine structure anomalies (the Bohr-Weisskopf effect) over long isotopic chains. The hfs anomalies result from the effect of the spatial distribution of the nuclear magnetization on the atomic hfs interaction. Constructional details of the system are described: emphasis is placed on the measurement of nuclear g-factors by a triple resonance, laser state selected, ABMR method. A precision better than 10−4 for gI values has been obtained in stable atomic b…

PhysicsNuclear and High Energy PhysicsIsotopechemistry.chemical_elementThermal ionizationMass spectrometryLaserlaw.inventionBohr modelNuclear physicsMagnetizationsymbols.namesakechemistrylawCaesiumsymbolsPhysics::Accelerator PhysicsPhysics::Atomic PhysicsDetectors and Experimental TechniquesAtomic physicsNuclear ExperimentInstrumentationHyperfine structureNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Das Vorzeichen der Hyperfeinstruktur-Aufspaltung des 3d 5 4s 2 6 S 5/2-Grundzustandes des Mn55

1962

Using a double Fabry-Perot interferometer and an atomic-beam light source, the sign of the hyperfine-structure splitting of the 3d 5 4s 2 6 S 5/2 ground state of Mn55 has been determined to be negative. The absolute value of the splitting previously has been measured byWoodgate andMartin.

PhysicsNuclear and High Energy PhysicsLight sourceAbsolute valueAtomic physicsGround stateHyperfine structureSign (mathematics)Zeitschrift für Physik
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Charge-radius change and nuclear moments in the heavy tin isotopes from laser spectroscopy: Charge radius ofSn132

2005

Laser spectroscopy measurements have been carried out on the neutron-rich tin isotopes with the COMPLIS experimental setup. Using the $5{s}^{2}5{p}^{2\phantom{\rule{0.3em}{0ex}}3}{P}_{0}\ensuremath{\rightarrow}5{s}^{2}5p6s\phantom{\rule{0.3em}{0ex}}{}^{3}{P}_{1}$ optical transition, hyperfine spectra of $^{126\ensuremath{-}132}\mathrm{Sn}$ and $^{125,127,129\ensuremath{-}131}\mathrm{Sn}{}^{m}$ were recorded for the first time. The nuclear moments and the mean square charge radius variation ($\ensuremath{\delta}\ensuremath{\langle}{r}_{c}^{2}\ensuremath{\rangle}$) were extracted. From the quadrupole moment values, these nuclei appear to be spherical. The magnetic moments measured are thus co…

PhysicsNuclear and High Energy PhysicsMagnetic moment010308 nuclear & particles physicsCharge density7. Clean energy01 natural sciencesSpectral lineMean field theoryCharge radius0103 physical sciencesQuadrupoleIsotopes of tinAtomic physics010306 general physicsHyperfine structurePhysical Review C
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Large Odd-even Radius Staggering In The Very Light Platinum Isotopes From Laser Spectroscopy

1999

Laser spectroscopy measurements have been carried out on very-neutron-deficient platinum isotopes with the COMPLIS experimental setup. Using the ${5d}^{9}{6s}^{3}{D}_{3}\ensuremath{\rightarrow}{5d}^{9}{6p}^{3}{P}_{2}$ optical transition, hyperfine spectra of ${}^{182,181,180,179,178}\mathrm{Pt}$ and ${}^{183}{\mathrm{Pt}}^{m}$ were recorded for the first time. The variation of the mean square charge radius between these nuclei, the magnetic moments of the odd isotopes, and the quadrupole moment of ${}^{183}{\mathrm{Pt}}^{m}$ were thus measured. A large deformation change between ${}^{183}{\mathrm{Pt}}^{g}$ and ${}^{183}{\mathrm{Pt}}^{m},$ an odd-even staggering of the charge radius, and a d…

PhysicsNuclear and High Energy PhysicsMagnetic moment010308 nuclear & particles physicsNuclear Theorychemistry.chemical_elementCharge density[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]XX7. Clean energy01 natural sciencesSpectral linechemistryCharge radius0103 physical sciencesQuadrupoleAtomic physics010306 general physicsSpectroscopyPlatinumHyperfine structure
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Spin, moments, and mean square nuclear charge radius ofSr77

1992

The neutron deficient $^{77}\mathrm{Sr}$ nucleus was studied by fast ion beam collinear laser spectroscopy with a detection scheme based on optical pumping, state selective neutralization, and atom counting. From the measured hyperfine splitting and isotope shift of the Sr II transition 5s $^{2}$${\mathit{S}}_{1/2}$\ensuremath{\rightarrow}5p $^{2}$${\mathit{P}}_{3/2}$ the nuclear spin I=5/2, the nuclear moments \ensuremath{\mu}=-0.348(4)${\mathrm{\ensuremath{\mu}}}_{\mathit{N}}$, ${\mathit{Q}}_{\mathit{s}}$=1.40(11) b, and the change in mean square charge radius \ensuremath{\delta}〈${\mathit{r}}^{2}$${\mathrm{〉}}^{88,77}$=0.248(12) ${\mathrm{fm}}^{2}$ were deduced. These ground-state proper…

PhysicsNuclear and High Energy PhysicsMagnetic momentCharge radiusAtomCharge densityAtomic physicsGround stateSpin (physics)Hyperfine structureEffective nuclear chargePhysical Review C
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Nuclear ground-state spins and magnetic moments ofMg27,Mg29, andMg31

2008

The ground-state spins and magnetic moments of neutron-rich {sup 27}Mg, {sup 29}Mg, and {sup 31}Mg were measured for the first time with laser and {beta}-NMR spectroscopy at ISOLDE/CERN. The hyperfine structure of {sup 27}Mg--observed in fluorescence--confirms previous assignments of the spin I=1/2 and reveals the magnetic moment {mu}{sub I}({sup 27}Mg)=-0.4107(15){mu}{sub N}. The hyperfine structure and nuclear magnetic resonance of optically polarized {sup 29}Mg--observed in the asymmetry of its {beta} decay after implantation in a cubic crystal--give I=3/2 and {mu}{sub I}({sup 29}Mg)=+0.9780(6){mu}{sub N}. For {sup 31}Mg they yield together I=1/2 and {mu}{sub I}({sup 31}Mg)=-0.88355(15){…

PhysicsNuclear and High Energy PhysicsMagnetic momentIsland of inversionHadronAtomic physicsNucleonGround stateIsotopes of magnesiumHyperfine structureRadioactive decayPhysical Review C
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